Lezione-17

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Sound absorption
16 November 2012
Sound Absorption
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Sound against a wall
• Balance of sound energy
impinging over a wall
• The energy balance shows
three main fluxes:
– Reflected
– Absorbed
– Transmitted
• Hence three coefficients are
defined, as the ratios with the
impinging energy
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Sound Absorption
r+a+t =1
2
Materials: sound insulating & sound absorbing
Sound absorbing materials must not be confused with sound insulating
materials:
Sound Insulating material:
Heavy and stiff, minimizes
transmitted power “Wt”.
the
Sound Absorbing material:
Soft and porous, minimizes
reflected power “Wr”.
16 November 2012
the
Sound Absorption
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Sound absorption = weak reflection
• If the surface is large compared to wavelength, the
reflection happens specularly, as a light ray (Snell’s
Law).
S
S’
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Sound Absorption
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Sound absorption = weak reflection
Regarding sound absorption
IT DOES NOT MATTER
if sound energy is dying inside the wall or is passing through
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Sound Absorption
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Sound absorbing materials: generalities (1)
When the the noise source is in the same room as the receiver, the noise level
can be reduced in three ways:
• reducing the sound power radiated by the source,
• bringing the receiver far away from the source ( r < rc),
• reducinhg the reflected energy (r > rc).
The latest effect is obtained by increasing the equivalent absorption area A,
which is given by:
• A =  i Si
( m2 )
where Si and i are respectively area and absorption coefficient of the i-th
surface surrounding the room.
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Sound Absorption
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Sound absorbing materials: generalities (2)
Inside the purely reverberant sound field (r >> rc), the sound level reduction
DL caused by the increase of sound absorption is given by:
• DL (f) = 10 log (A2/ A1)
(dB)
where 1 and 2 refer to the values before and after the introduction of the
absorbers.
Sound absorbing materials are usually classified in the following categories:
a) porous materials,
b) acoustic resonators,
c) vibrating panels,
d) hybrid systems.
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Sound Absorption
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SOUND ABSORBING MATERIALS
Porous materials
Suspended ceiling, hanging
under the structure
Foam attached directly to the
structure
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Sound Absorption
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SOUND ABSORBING MATERIALS
Absorption coefficient vs. frequency & thickness
Increasing the thickness of a porous layer attached directly on a rigid wall
improves absorption at low frequency
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Sound Absorption
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SOUND ABSORBING MATERIALS
Effect of distance from a rigid wall
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Sound Absorption
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SOUND ABSORBING MATERIALS
Acoustic
resonators
f0 
c0
2
r
2
Scheme of an Helmoltz’s resonator
 

V l 

2r 

c0 : sound speed (m/s)
r : neck’s radius (m)
l : neck’s length (m)
V : volume of rear cavity (m3)
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Sound Absorption
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Effect of damping material inside
SOUND ABSORBING MATERIALS
Vibrating panels
Scheme of a vibrating panel
f0 =
60
(s × d )
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 : surface density of panel (kg/m2)
d : distance panel – wall (m)
Sound Absorption
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SOUND ABSORBING MATERIALS
Hybrid systems
Schemes of hybrid systems
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Sound Absorption
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SOUND ABSORBING MATERIALS
Vibrating panels
Hybrid systems
Resonators
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Sound Absorption
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Example - Casa della Musica
Helmoltz Resonators
Porous panels
Vibrating panels
“Bass Trap”
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Sound Absorption
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Sound Scattering Coefficient s
Wdiff
s=
Wdiff +Wspec
• On a rough surface, a fraction s of the reflected energy will
be radiated diffusely, while the remaining fraction 1-s will be
radiated specularly
Specular component
Wspec =Winc·(1-α) · (1s)
Diffused component
Wdif =Winc·(1-α) · s
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Sound Absorption
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Acoustic diffusors
• Most diffusing panels are done by:
• pseudo-random cavities
• 2D and 3D scattering versions
• Curved surfaces
Reference brand: RPG Diffusor Systems
(http://www.rpginc.com)
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Acoustic diffusors
Curved panels are often used for building acoustical shells in
theatres
Reference brand: Wenger
(http://www.wengercorp.com)
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Sound Absorption
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